4th Week: Decays, Tunneling and Cross Sections

Nuclear Radiation

Figure 1. A table of known stable and radioactive nuclides

When looking at the table of nuclides it is obvious that the valley of stability is only a small percentage of all known nuclei. So most nuclei are considered unstable. To become stable these nuclides emit ionizing particles and radiation, resulting in a loss of energy from the original nuclei. This Process is called radioactive decay.

Alpha Decay and Fission

Alpha decay is the transformation of a parent nucleus to a daughter nucleus through the emission of a helium nucleus. This decay is usually seen in heavier elements with too many protons. This causes excessive repulsion due to the coulomb force. In an attempt to get rid of this excessive repulsion the nucleus emits an alpha particle.

$_{Z}^{A}{\textrm {X}}\to \;_{Z-2}^{A-4}{\textrm {Y}}+\;_{2}^{4}{\textrm {He}}$

Beta Decay

Figure 1.

There are three types of Beta decays, $\beta ^{-}$-decay, $\beta ^{+}$-decay, and electron capture. All three of these decays can be characterized by $\Delta A=0$ and $\left|\Delta Z\right|=1$.

The first one, $\beta ^{-}$decay, occurs when a nucleus with an over abundance of neutrons transforms to a more stable nucleus by emitting an electron. This process can be denoted as:

$_{Z}^{A}{\textrm {X}}\to \;_{Z+1}^{A}{\textrm {Y}}+\;e^{-}$

From electric-charge conservation, the proton number in such decays is increased by one unit.

Likewise, a $\beta ^{+}$-decay occurs when a proton-rich nucleus emits a positron, therefore reducing the nuclear charge by one.

$_{Z}^{A}{\textrm {X}}\to \;_{Z-1}^{A}{\textrm {Y}}+\;e^{+}$

Gamma Decay

$E_{\alpha }=E_{centerofmass}{\frac {M_{product}+M_{reaction}}{M_{reaction}}},\;\;\;\;E_{centerofmass}=E_{\alpha }{\frac {M_{reaction}}{M_{reaction}+M_{product}}}$